|Numéro de publication||US8035028 B2|
|Type de publication||Octroi|
|Numéro de demande||US 11/868,493|
|Date de publication||11 oct. 2011|
|Date de dépôt||6 oct. 2007|
|Date de priorité||9 oct. 2006|
|État de paiement des frais||Payé|
|Autre référence de publication||CN101657904A, CN101657904B, EP2084751A2, EP2084751A4, US20080289684, US20120017988, WO2008057687A2, WO2008057687A3|
|Numéro de publication||11868493, 868493, US 8035028 B2, US 8035028B2, US-B2-8035028, US8035028 B2, US8035028B2|
|Cessionnaire d'origine||Solexel, Inc.|
|Exporter la citation||BiBTeX, EndNote, RefMan|
|Citations de brevets (121), Citations hors brevets (37), Référencé par (17), Classifications (18), Événements juridiques (6)|
|Liens externes: USPTO, Cession USPTO, Espacenet|
This application claims the benefit of provisional patent applications 60/828,678 filed on Oct. 9, 2006 and 60/886,303 filed on Jan. 24, 2007, which are hereby incorporated by reference.
This disclosure relates in general to the field of photovoltaics and solar cells, and more particularly to three-dimensional (3-D) Thin-Film Solar Cells (TFSCs) and methods for manufacturing same. Even more particularly, the presently disclosed subject matter relates to pyramidal 3-D TFSCs and methods for manufacturing same.
Renewable, high-efficiency, and cost-effective sources of energy are becoming a growing need on a global scale. Increasingly expensive, unreliable, and environmentally-risky fossil fuels and a rising global demand for energy, including electricity, have created the need for alternate, secure, clean, widely available, cost-effective, environmentally-friendly, and renewable forms of energy. Solar photovoltaic (PV) electricity generation using solar cells is uniquely suited to meet the needs of residential, commercial, industrial, and centralized utility applications. Key attributes that make solar energy attractive are the abundant, worldwide, point-of-use supply of sunlight, environmental friendliness, scalability (from milliwatts to megawatts), secure point-of-use generation of solar electricity, and excellent distributed energy economics. The sun provides more energy to the earth in one hour than the annual energy consumption of the entire world. Much of the earth's surface receives a significant amount of annual sun-hours which may be effectively harnessed for clean and secure electricity generation. A key driver for this market pull is a rising public awareness of environmentally-benign technologies. However, due to relatively low solar cell efficiencies (e.g., less than 12% for most thin-film technologies and roughly 12% to 18% for most crystalline silicon solar cell technologies), high costs of raw materials (e.g., silicon for crystalline silicon wafer solar cells) and manufacturing processes, limitations on cost-effective and efficient electrical storage, and a general lack of infrastructure to support solar cell proliferation, to date there has been limited use of this energy solution (currently, electricity generation by solar photovoltaics accounts for less than 0.1% of total worldwide electricity generation).
For commercial applications, cost of energy to the end-user (e.g., in cents/kWh for electricity) should be sufficiently low and comparable to or even better than that from utility grids using conventional electricity generation sources. The solar photovoltaic electricity generation, which currently accounts for less than 0.1% of the global electricity generation, may be substantially expanded if it achieves cost parity with conventional grid electricity. As the costs of solar cells and modules (typically expressed as $/Wp) are reduced, grid-tied solar photovoltaic applications are gaining acceptance at an accelerated pace, making them an attractive option for significant proliferation in electricity generation.
In the price-sensitive solar cell market, two principal technology options exist. On the one hand, crystalline silicon (c-Si) wafers may serve as the basis for solar cell formation (currently accounting for more than 90% of the solar PV market). On the other hand, thin-film (amorphous and polycrystalline) technologies using silicon and other semiconductor absorber materials (such as amorphous silicon, CdTe, or CIGS) may offer significant cost advantages compared to crystalline silicon wafer-based solar cells. These different approaches are at opposite ends of the price-performance scale. Crystalline silicon wafers offer higher performance, but at higher costs (due to the relatively high cost of starting monocrystalline and multicrystalline silicon wafers). Thin-film technologies may offer lower manufacturing costs, but typically at lower performance levels (i.e., lower efficiencies). For both approaches, the price-per-watt typically increases as cell efficiencies rise (due to higher material and/or manufacturing costs).
Due to a rapid annual growth rate of more than 40% during the past ten years and the concurrent demands for silicon material by both semiconductor microelectronics and solar PV industries, the solar PV industry has been experiencing a shortage of polysilicon feedstock supply. The polysilicon feedstock shortage has significantly constrained the solar PV industry growth, particularly during the past several years. In fact, the solar cell industry currently consumes over half of the worldwide production of high-purity polysilicon feedstock. Within the last few years, the contract price of polysilicon has increased from roughly $30/kg to roughly $85/kg, with spot prices exceeding $250/kg. This has led to large increases in the price of monocrystalline and multicrystalline silicon wafers, which now account for roughly half of the total solar module manufacturing cost.
The trend in the mainstream crystalline silicon (c-Si) wafer solar cell industry has been to scale down wafer thicknesses to below 200 microns (in order to reduce the amount of silicon material in grams used per watt of solar cell rated peak power). For example, monocrystalline silicon wafer solar cells are projected to scale down to a thickness of roughly 120 microns by 2012, from a current wafer thickness of roughly 200 microns. Multicrystalline silicon wafer solar cells are projected to scale down to a thickness of roughly 180 microns by 2012, from a current average wafer thickness of roughly 260 microns. This wafer thickness reduction, however, presents additional challenges related to mechanical rigidity, manufacturing yield, and solar cell efficiency. Despite its high cost, crystalline silicon (c-Si) technology still dominates the solar cell market, mainly due to higher efficiencies and synergies with the established microelectronics industry and supply chain. Currently, c-Si accounts for slightly over 90% of the solar cell market (95% when ribbon silicon is included).
Historically, crystalline silicon solar cells have achieved a 20% cost reduction for each doubling of cumulative global cell production (measured in megawatts or MWp and gigawatts or GWp). It is projected that through innovative cost reduction and efficiency enhancement methods, the cost of electricity derived from grid-connected rooftop solar photovoltaic modules may become comparable to the cost of electricity purchased from the utility grid in five to ten years. A 2005 survey of the commercially available monocrystalline silicon and multicrystalline silicon solar modules reports the solar module efficiencies then in the range of 9.1% to 16.1%, with a median efficiency value of about 12.5%. Commercial crystalline silicon modules usually show a rapid initial efficiency degradation of 1% to 3% (relative) due to various effects, including photodegradation effects in wafered solar cells (e.g., wafer minority carrier lifetime degradation). Monocrystalline silicon wafer solar cell efficiencies are projected to increase to roughly 20.5% by 2012, from a current efficiency of roughly 16.5% (leading-edge commercially available monocrystalline silicon solar cell and solar module efficiencies are currently about 21.5% and 18%, respectively). Multicrystalline silicon wafer solar cell efficiencies are projected to increase to roughly 18% by 2012, from a current efficiency level of roughly 15.5%.
State-of-the-art crystalline silicon solar cell manufacturing currently uses about 10 grams of high-purity polysilicon feedstock per peak watt (g/Wp), resulting in a polysilicon feedstock material cost of about $0.85/Wp (assuming a polysilicon price of $85/kg). Over the next five years, the projected trends of solar cell wafer thickness reduction (e.g., to less than 200 micron wafers) and a long-term assumed price of about $20/kg for solar-grade polysilicon may reduce the polysilicon feedstock cost (in g/Wp) by about a factor of four to eight to about $0.10/Wp to $0.20/Wp. Thus, any competing solar cell technologies should benchmark their manufacturing cost goals against this reduced raw material cost number. For a given cell efficiency, silicon wafer thickness reduction presents a prime opportunity for solar cell cost reduction by reducing the amount of polysilicon feedstock consumed per watt of peak solar power.
The cost associated with wire saws, amounting to about $0.25/Wp for current silicon solar cells provides another wafer-related cost component for silicon wafer solar cells. Innovative and cost-effective technologies that eliminate the kerf losses associated with sawing and slicing should further facilitate silicon solar cell cost reductions. It is projected that the wafer-based crystalline silicon solar module manufacturing cost (which is currently on the order of $2.10 per watt to more than $2.70 per watt) may be reduced to the range of roughly $1.50/Wp to $1.80/Wp by the year 2012, in part due to wafer sawing kerf loss reduction to roughly 130 microns by 2012 from the current value of roughly 200 microns. The overall cost reductions for wafer-based crystalline silicon solar cells may come from various sources including: lower cost polysilicon feedstock, thinner wafers, higher cell-level efficiencies, reduced wafer sawing kerf losses, and increased economy of scale or manufacturing volume.
State-of-the-art silicon wafer solar cell fabrication facilities (“solar fabs”) typically produce 125 mm×125 mm up to 156 mm×156 mm solar cells today. The trend in crystalline silicon wafer solar cells is toward thinner and larger wafers. The monocrystalline and cast (as well as ribbon) multicrystalline silicon solar cell wafer thicknesses in leading-edge solar cells used for power generation modules are projected to be reduced to around 150 and 200 microns, respectively, by around 2009-2010. Any cost-effective, high-efficiency, innovative silicon solar cell technology which enables a substantial reduction of the silicon material consumption (e.g., wafer or film thickness) per Wp of cell power compared to the above-mentioned current and projected 2009-2010 numbers may offer significant promise as a viable commercial solar cell technology for solar photovoltaic applications (e.g., residential, commercial, and industrial rooftop as well as large-scale centralized utilities electrical power generation applications).
Higher solar cell efficiencies have favorable effects on the entire solar cell value chain and levelized cost of energy (LCOE in $/kWh) due to reduced material consumption and cost as well as reduced balance-of-system (BOS) costs (e.g., area-related solar module installation and inverter costs). The current mainstream commercial crystalline solar cells provide efficiencies on the order of 14% to 17%. It is expected that the projected crystalline silicon solar cell efficiencies in commercial solar cells may approach around 19% and 17% for monocrystalline and multicrystalline silicon solar cells, respectively, by the year 2009. A key area for new solar cell business opportunities is development of innovative cell structures and simplified process flows which may drive efficiencies up while lowering overall solar cell and module manufacturing costs. For alternative (e.g., thin-film PV) approaches to succeed over the mainstream wafer-based crystalline silicon solar cell technologies, they should provide higher efficiencies at even lower manufacturing costs compared to the projected efficiency and cost numbers for the mainstream wafer-based crystalline silicon solar cells when the new technology is fully commercialized.
Economy-of-scale fab cost reduction associated with high-volume solar fab capacities is a key factor impacting LCOE. The state-of-the-art high-volume solar photovoltaic fabs have annual production capacities on the order of or in excess of 50 MWp to 100 MWp (MWp=1 million Wp). High-volume solar photovoltaic fab capacities are expected to increase substantially to annual production rates of several hundred MWP or even approaching 1 GWp (GWp=1 billion Wp) in the coming decade. While very-high-volume solar fabs in the range of 100 MWp to 1 GWp should facilitate longer term cost reductions (including LCOE) through high-volume manufacturing economies of scale, the relatively high initial fab investment costs, which may easily exceed $100M, may impose certain limits on solar photovoltaic fab construction options. Ideally, the preference may be to develop innovative crystalline silicon solar cell designs and simplified manufacturing processes which facilitate substantial manufacturing cost reductions in solar cells and modules even in smaller-scale (and less capital intensive) fabs with modest production volumes (e.g., annual production volumes in the range of 5 MWp to 50 MWp). This type of technology would allow for modest-volume solar photovoltaic fabs with modest fab setup and operation costs. Reduced fab setup and operation costs would further facilitate global proliferation of cost-effective solar modules, enabling construction of a multitude of very affordable modest-volume fabs (in contrast to having to set up very expensive high-volume fabs in order to achieve sufficient economy of scale for manufacturing cost reduction). Of course, an innovative solar cell technology that meets the above-mentioned criteria for cost-effective, modest-volume fabs (i.e., meeting the LCOE roadmap requirements even at modest production volumes in low-cost fabs set up for simplified solar cell processing), may also be applicable to very-high-volume (e.g., greater than 100 MWp) solar fabs. Such solar photovoltaic fabs can take further advantage of the economies of scale associated with increased volume.
Thin-film solar cell (TFSC) technologies (e.g., amorphous silicon, CdTe, and CIGS) require little absorber material (usually much less than 10 microns in thickness) to absorb typical standard “Air Mass 1.5” (AM-1.5) solar illumination due to absorption bands that are well matched to the solar spectrum. The TFSC absorber material may be deposited on inexpensive substrates such as glass or flexible metallic or non-metallic substrates. TFSCs typically offer low cost, reduced module weight, reduced materials consumption, and a capability for using flexible substrates, but are usually much lower in efficiency (e.g., usually 5% to 12%). In the case of prior art thin crystalline silicon films, there are a number of major problems and challenges with the use of flat silicon films (such as epitaxially growth silicon films with thicknesses below 50 microns) for low-cost, high-performance solar cells. These include: relatively low solar module efficiencies (typically 7% to 12%), field degradation of module efficiencies, scarce and expensive absorber materials (e.g., In and Se for CIGS and Te for CdTe), limited validation of system field reliability, and adverse environmental impact of non-silicon technologies such as CIS/CIGS and CdTe.
With regard to the prior art crystalline silicon (c-Si) thin-film solar cell (TFSC) technology, there are difficulties associated with sufficient surface texturing of the thin silicon film to reduce surface reflectance losses, while reducing the crystalline silicon film thickness. This places a limit on the minimum flat (co-planar) monocrystalline silicon thickness due to production yield and cell performance (efficiency) considerations. In the case of a flat or co-planar film, it is essential to use surface texturing since the reflectance of an untextured crystalline silicon film is quite excessive (can be greater than 30%) and results in substantial optical reflection losses and degradation of the external quantum efficiency. Thus, reduction of reflectance-induced photon losses in co-planar epitaxial silicon films requires effective surface texturing which itself places a limit on the minimum epitaxial silicon layer thickness. Depending on the film surface texturing requirements and processes, the minimum crystalline silicon layer thickness may be on the order of at least 10 microns (so that the texturing process does not break through any portions of the crystalline silicon layer).
In addition, substantially reduced mean optical path lengths in thin planar crystalline silicon films result in reduced photon absorption, particularly for photons with energies near the infrared bandgap of silicon (800 to 1100 nanometers), resulting in reduced solar cell quantum efficiency (reduced short-circuit current or Jsc). This results in serious degradation of the solar cell efficiency due to reduced cell quantum efficiency and reduced Jsc. For instance, in a co-planar (flat) crystalline silicon absorber layer with thickness of 20 microns, a solar light beam impacting the cell at a near-normal angle would have an effective path length equal to the film thickness, far too short for the solar radiation photons with energies near the infrared bandgap of silicon (i.e., with wavelengths of roughly 800 to 1100 nanometers) to be absorbed effectively in the silicon thin film. In fact, a reduction of the active cell silicon thickness to below roughly 50 microns results in appreciable reduction of Jsc and the resulting solar cell efficiency, with this degradation effect rapidly accelerating when the silicon film thickness is reduced below roughly 20 microns. Thus, a co-planar thin crystalline silicon film may also require effective light trapping using both top surface texturing and rear surface back reflection of the light exiting the back surface of the crystalline silicon film in order to create effective optical path lengths equal to a large multiple of the crystalline silicon film thickness.
The prior art technologies using this approach mostly use either back reflection through internal reflection of the light at the crystalline silicon film/silicon substrate, or reflection from a blanket backside contact (such as a back surface field aluminum contact/mirror). The back reflectance provided by these techniques may not be great (e.g., roughly 70% effective near-IR rear reflectance), constraining the performance gain that would have otherwise been achieved by an optimal back reflector. The problem with this approach is that the primary incident beam always passes the crystalline silicon film only once. Any subsequent second passes of the primary incident beam photons are dependent on the back surface reflection.
There is also the problem of lack of rigidity and mechanical support of the thin film during cell and module processing steps. This problem relates to the mechanical strength of a large-area (e.g., 200 mm×200 mm) thin silicon film. It is well known that reducing the large-area crystalline silicon wafer thickness to below 100 microns results in a substantial loss of cell substrate mechanical strength/rigidity, and such thin wafers tend to be flexible and very difficult to handle without breakage during cell fabrication process flow.
Large-area, co-planar (flat) crystalline silicon films thinner than, for instance, 50 microns must be properly mounted and supported on a cost-effective support or handle substrate in order to achieve acceptable yield for solar cell and module manufacturing. One approach is to grow and retain the thin epitaxial film on a relatively low-cost (e.g., metallurgical-grade) silicon substrate (over which the epitaxial layer is grown); however, this approach suffers from some inherent problems constraining the ultimate solar cell efficiency. Another approach is to release or lift off the epitaxial silicon film from its (reusable) parent silicon substrate and subsequently place it on a cheaper non-silicon support or handle substrate to provide mechanical strength through the solar cell process flow. This approach may suffer from any thermal coefficient of expansion (TCE) mismatch between the support/handle substrate and silicon film during any high-temperature oxidation and anneal processes, as well as potential contamination of the thin epitaxial silicon film from the non-silicon support substrate (both creating possible manufacturing yield and performance/efficiency degradation problems).
The cost of the monocrystalline silicon film growth process using silicon epitaxy, particularly for thicker epitaxial films with thicknesses in excess of 30 microns is an additional issue which should be addressed. Using a relatively small epitaxial film thickness (in one embodiment, much below 30 microns) may lower the cost of epitaxy to an attractive range. However, this would present various challenges for fabrication of planar silicon thin-film solar cells. As stated, thinner co-planar (flat) epitaxial films (e.g., in the range of much less than 30 microns) produce a number of problems and challenges, including a lack of film mechanical strength, constraints limiting effective surface texturing of thin silicon films for low surface reflectance and reduced optical reflectance losses, relatively short optical path lengths, and reduced cell quantum efficiencies. Effective light trapping is essential for enhanced thin-film c-Si solar cell efficiencies. The requirement for effective light trapping is based on a combination of front surface texturing and back surface mirror, while achieving sufficiently low surface recombination velocities (for high cell efficiencies). This is very difficult to achieve in the co-planar (flat) c-Si thin film solar cells.
High-performance c-Si thin-film solar cells require some patterning steps or patterned processing steps (e.g., for formation of selective emitter, frontside emitter or backside emitter wrap-through metallization contacts, backside base metallization contacts, etc.). These patterning steps are usually achieved using photolithography, screen printing, and/or shadow-mask deposition (e.g., shadow-mask sputtering or evaporation) processes. The use of photolithography and/or screen printing and/or shadow-mask deposition patterning steps usually increases the manufacturing process flow complexity and cost, and may also detrimentally impact the fabrication yield as well as the ultimate achievable solar cell efficiency.
Therefore a need has arisen for a thin-film solar cell (TFSC) which corrects the problems identified above.
Yet a further need exists to address shortcomings of existing mainstream c-Si solar cell technology. This includes reducing the amount of polysilicon feedstock consumed per peak watt of solar power, and eliminating the kerf losses associated with sawing and slicing; thus, substantially reducing the overall solar cell manufacturing cost.
A further need exists for innovative solar cell structures and simplified process flows, increasing cell and module efficiencies while significantly lowering the overall solar cell and module manufacturing costs. A still further need exists for innovative c-Si solar cell designs and simplified self-aligned manufacturing processes which facilitate substantial solar cell and module cost reduction even in fabs with modest production volumes, enabling low to mid-volume solar cell fabs with modest fab setup and operation costs (thus, achieving economies of scale for manufacturing cost reduction at substantially lower fab volumes than the prior art fabs).
A still further need exists to address shortcomings of existing TFSC technology. This includes addressing difficulties associated with sufficient surface texturing of the thin planar silicon films to reduce surface reflectance losses, which currently places a limit on the minimum flat (co-planar) crystalline silicon thickness due to production yield and cell performance considerations. A still further need exists for effective light trapping based on a combination of front surface texturing and back surface mirror, while achieving low surface recombination velocities (for high cell efficiencies).
A still further need exists to address additional shortcomings of existing TFSC technologies. This includes the problem of lack of rigidity and mechanical support of the thin film substrate during cell and module processing steps, thus, necessitating the use of support or handle substrates (made of silicon or another material) for the TFSC substrates. This further includes the cost of the epitaxial silicon film growth process, particularly for thicker epitaxial films required for planar crystalline silicon TFSCs. This further includes the requirement of multiple photolithography and/or screen printing and/or shadow-mask processing/patterning steps which usually increase the manufacturing process flow complexity and cost, and may also detrimentally impact the fabrication yield as well as the ultimate achievable solar cell efficiency.
In accordance with the present disclosure, pyramidal three-dimensional thin-film solar cells (3-D TFSCs) are provided. The pyramidal 3-D TFSCs of the disclosed subject matter substantially eliminate or reduce disadvantages and problems associated with previously developed TFSCs, both in terms of efficiency and manufacturing cost.
According to one aspect of the disclosed subject matter, there is provided a pyramidal 3-D TFSC, comprising a pyramidal 3-D TFSC substrate, wherein said pyramidal 3-D TFSC substrate comprises a plurality of pyramid-shaped unit cells.
According to another aspect of the disclosed subject matter, there is provided a pyramidal 3-D TFSC, comprising a pyramidal 3-D TFSC substrate, wherein said pyramidal 3-D TFSC substrate comprises a plurality of unit cells with pyramid-shaped cavities.
Optionally, the pyramidal 3-D TFSCs may be mounted on a rear mirror for improved light trapping and conversion efficiency.
According to still another aspect of the disclosed subject matter, there is a provided a pyramidal 3-D TFSC. The pyramidal 3-D TFSC comprises a pyramidal 3-D TFSC substrate with emitter junction regions and doped base regions. The pyramidal 3-D TFSC further includes emitter metallization regions and base metallization regions. The pyramidal 3-D TFSC substrate comprises a plurality of pyramid-shaped unit cells.
More specifically, the disclosed subject matter includes a pyramidal 3-D TFSC substrate made of silicon, and even more specifically made of crystalline silicon.
More specifically, the disclosed subject matter includes a pyramidal 3-D TFSC substrate with a pyramid-array design, and even more specifically, a hexagonal-pyramid design or a polygon-pyramid design, among others.
More specifically, the disclosed subject matter includes pyramidal 3-D TFSC with an integrated rear mirror or a detached rear mirror.
These and other advantages of the disclosed subject matter, as well as additional novel features, will be apparent from the description provided herein. The intent of this summary is not to be a comprehensive description of the claimed subject matter, but rather to provide a short overview of some of the subject matter's functionality. Other systems, methods, features and advantages here provided will become apparent to one with skill in the art upon examination of the following FIGURES and detailed description. It is intended that all such additional systems, methods, features and advantages be included within this description, be within the scope of the accompanying claims.
The features, nature, and advantages of the disclosed subject matter may become more apparent from the detailed description set forth below when taken in conjunction with the drawings in which like reference characters identify correspondingly throughout and wherein:
Preferred embodiments of the present disclosure are illustrated in the drawings, like numbers being used to refer to like and corresponding parts of the various drawings. The innovative solar cell designs and technologies of the current disclosure are based on the use of a three-dimensional (3-D), self-supporting, doped (in one embodiment, in-situ-doped) semiconductor thin film, deposited on and released from a reusable crystalline (embodiments include monocrystalline or multicrystalline silicon) semiconductor template.
A preferred semiconductor material for the 3-D TFSC substrate is crystalline silicon (c-Si), although other semiconductor materials may also be used. One embodiment uses monocrystalline silicon as the thin film semiconductor material. Other embodiments use multicrystalline silicon, polycrystalline silicon, microcrystalline silicon, amorphous silicon, porous silicon, and/or a combination thereof. The designs here are also applicable to other semiconductor materials such as germanium, silicon germanium, silicon carbide, a crystalline compound semiconductor, or a combination thereof. Additional applications include copper indium gallium selenide (CIGS) and cadmium telluride semiconductor thin films.
The 3-D TFSC designs and production technologies as well as associated module structures and assembly approaches of this disclosure effectively overcome the above-mentioned problems and challenges and enable cost-reduced fabrication of very-high-efficiency solar cells and modules using self-aligned cell process flows without the use of any photolithography patterning or screen printing or shadow-mask deposition process steps during cell fabrication (i.e., during 3-D TFSC substrate and cell fabrication after fabrication of the reusable 3-D template). The 3-D TFSC technologies of this disclosure are based on the formation of a 3-D pyramid-array TFSC substrate structure on a low-cost reusable template and its subsequent release and lift-off from the template to form a free-standing, self-supporting 3-D thin-film semiconductor substrate structure.
The current disclosure combines the benefits of TFSC fabrication on a proven high-efficiency crystalline silicon (c-Si) platform. The 3-D c-Si TFSC designs and technologies of this disclosure enable significant advancements in the areas of c-Si solar cell and module efficiency enhancement as well as manufacturing cost reduction. Based on innovative thin-film process steps, dependence on an expensive and constrained silicon wafer supply-chain is eliminated. Some of the unique advantages of the cells designs and technologies of this disclosure which enable achieving ultra-high-efficiency at reduced manufacturing cost are substantial decoupling from the traditional solar PV silicon supply chain, performance enhancement, cost reduction, and reliability improvement.
The disclosed subject matter improves solar cell efficiency by using a 3-D c-Si film as an absorber layer in conjunction with highly efficient light trapping. Use of the crystalline silicon absorber layer leverages known solar cell manufacturing techniques and supply chain, while reducing absorber layer thickness (e.g., reduced by a factor of ten or more compared to silicon wafers used for wafer-based solar cells). The disclosed method and system eliminates or substantially reduces photo-degradation and enhances open-circuit voltage (Voc) of cells. In addition, the disclosed method and system provides efficient frontside and rear side light-trapping in conjunction with a highly reflective rear mirror for maximum absorption of incident solar flux. Also, the disclosed method and system provides a selective emitter to enhance blue response and external quantum efficiency, with minimal shadowing of the cell and reduced ohmic losses due to a unique folded emitter metallization contact design and improved module assembly.
Manufacturing cost is reduced by decreasing silicon usage (by a significant factor, e.g., 3× to over 10×), with thinner deposited c-Si films also reducing the finished solar module energy payback time to less than 1 to 2 years. Manufacturing cost is further reduced by eliminating wire sawing and related kerf losses associated with mainstream solar cell wafer manufacturing technology. Manufacturing cost is still further reduced by using self-aligned processing without any lithography or patterning steps used during the substrate and cell fabrication process flow, and a reduced number of fabrication process steps, with improved yield and cycle time. Production cost is still further reduced by using a simplified interconnection and cell-module assembly process and lightweight monolithic modules.
Operational reliability is improved by using thinner silicon films, eliminating photo-degradation and reducing temperature coefficients. Operational reliability is further improved by using a simple distributed high-conductance electrical interconnection, minimizing field failures. Operational reliability is still further improved by eliminating module glass cover (for glassless module assembly), thus reducing cost and facilitating field installation and operation. Operational reliability is still further improved by reducing the number of manufacturing process steps and process variations using in-line manufacturing process control.
The current disclosure reduces the solar module cost per watt for the user (by at least 30% to 50%) and cuts balance-of-system (BOS) and installation costs for the integrators and installers. This may offer major benefits to the global grid-tied end-users and solar system installers and integrators. The current disclosure reduces the module integration and installation cost and installed solar cell system cost per Wp for the user, thereby lowering finished system cost per Wp. The current disclosure increases module efficiency, with higher module efficiency resulting in lower BOS cost. The lower installed solar cell system cost results in reduction of the economic break-even time to a lower fraction of the system lifetime, from roughly ½ to ⅓ for current best-of-breed c-Si solar cell systems to less than ¼ to ⅛ for the embodiments of this disclosure. The current disclosure reduces energy pay-back time (EPBT) from 3 to 7 years for best-of-breed c-Si solar cell systems to less than 1 to 2 years for the embodiments of this disclosure. Reduced EPBT substantially increases the net lifetime energy output (in kWh) for field-installed modules. The cell designs and module assemblies of this disclosure also provide stable degradation-free field operation over an extended time (e.g., 30 to 40 year life of the module), further increasing the net lifetime electrical energy output. Module manufacturing costs are expected to be 30% to 65% lower than that of the leading high-performance c-Si solar cells/modules at the time of market entry. This may shorten the ROI break-even time for the users compared to the current industry roadmap and projections. Further benefits include increased field performance stability and reliability and reduced environmental impact (non-toxic materials and shortened EPBT). Further, the cell and module designs of this disclosure are ideal for grid-tied applications where it is advantageous to maximize electricity generation from a limited building rooftop or façade area.
The absorber silicon film thickness of the current disclosure may be a value in the range of roughly 1 to 30 microns, where a thinner silicon layer is preferred for less material consumption (in one embodiment, in the range of 1 to 10 microns). Even after taking into account the effective surface area increase due to the 3-D geometric structure of the 3-D TFSC substrates, the 3-D TFSC substrates of this disclosure consume substantially less silicon material than the state-of-the-art wafer-based c-Si solar cells. Moreover, there are no sawing or kerf losses. Similarly, there is no requirement for saw damage removal since the 3-D crystalline silicon film is process-ready upon release from the reusable template. This substantially reduces the solar cell cost associated with silicon consumption. The self-supporting 3-D epitaxial silicon thin film is deposited on and released from a low-cost reusable crystalline (monocrystalline or multicrystalline) silicon substrate (template). The template may be reused numerous times before being reconditioned or recycled. The template may even be chosen from the much lower cost metallurgical-grade c-Si since any metallic impurities are prevented from contaminating the 3-D crystalline silicon film.
The following FIGURES show embodiments of 3-D TFSC substrate structures. The crystalline silicon film thickness is in the range of 2 to 30 microns, and preferably in the lower-end range of 2 to 10 microns. This is substantially less (by a factor of roughly 20× to 100×) than the state-of-the-art silicon solar cell wafer thickness (roughly 200 microns).
These 3-D TFSC substrates are used to fabricate 3-D pyramidal TFSCs.
When referring to the following FIGURES, the YY and ZZ axes are shown in
The following FIGURES show embodiments of 3-D TFSC substrate structures. The crystalline silicon film thickness is in the range of 2 to 30 microns, and preferably in the lower-end range of 2 to 10 microns. This is substantially less (by a factor of roughly 20× to 100×) than the state-of-the-art silicon solar cell wafer thickness (roughly 200 microns).
The following section details the process of using the 3-D TFSC substrates described above to fabricate 3-D thin-film solar cells (TFSCs). Specifically, the following FIGURES illustrate embodiments of process flows using alternative methods of fire-through metallization and selective plating metallization. These process flows do not use any photolithography or screen printing processes. The 3-D hexagonal-pyramid structural design of the solar cell substrate enables self-aligned processing throughout the entire cell process flow. The emitter and base contacts and metallized regions cover relatively small fractions of the frontside emitter and backside base areas, respectively. As indicated, selective emitter and base doping is achieved by self-aligned application of the n-type and p-type dopant pastes to the top and bottom of the 3-D hexagonal-pyramid substrate, preferably using double-sided roller coating method. The 3-D substrate is then cured and moves on to a belt furnace to form the n+ selective emitter on the frontside and the p+−doped base on the rear side of the 3-D substrate. A preferred n-type dopant source is phosphorus and a preferred p-type dopant source is boron.
Process flow 400 shown in
An alternative fire-through metallization process flow 430 is described in
Another alternative fire-through metallization process flow 460 is described in
As noted above,
Process flow 490 shown in
An alternative selective plating metallization process flow 520 is described in
Another alternative selective plating metallization process flow 550 is described in
Another alternative selective plating metallization process flow 580 is described in
Another alternative selective plating metallization process flow 610 is described in
The above process steps may be performed on integrated in-line process equipment. For example,
The 3-D TFSC substrate 642 is shown moving in 644 on input conveyor belt 646. The rotating top rollers 648, with top roller pads 650, apply a controlled downward force to coat the top ridges with n-type paste. The rotating rear rollers 652, with rear roller pads 654, apply a controlled upward force to coat the rear ridges with p-type paste. Multilayer materials may be coated on each side of the 3-D TFSC substrate by applying (or flowing) a different liquid or paste material to each roller on the top 648 and/or rear 652 set of rollers. The 3-D TFSC substrate 642 next moves into the curing area where the dopant liquid/paste layers are concurrently formed using a curing lamp 656 which uses IR or UV curing beams 658. The 3-D TFSC substrate 642 is next shown moving out 660 to the output conveyor belt 662, which may move the substrate 642 to an in-line diffusion furnace, where the n+ and p+ contacts and selective emitter regions are concurrently formed.
A similar roller coater setup may be properly configured and used for applying metal liquid/paste coatings (e.g., silver and/or aluminum liquid or paste sources), curing the metal liquid/paste source, and performing subsequent thermal anneal in an in-line atmospheric furnace (resistively-heated or lam-heated furnace) for fire-through metallization in order to form the emitter and base contact metallization (and whenever applicable, also to form the aluminum-doped p++ base contact regions).
The angled spray technique limits the vertical height of the liquid/paste coating to a portion of the ridges and prevents the liquid source from coating the inner parts of the hexagonal pyramid cavity sidewalls and/or rears. This type of in-line (or another drive method) processing system may also be used for applying metal source liquid (e.g., silver and/or aluminum source liquid) for fire-through metallization applications as well as applying liquid etchant for selective etching of dielectrics (e.g., oxide and/or solid dopant source layer) from the top and/or rear hexagonal-pyramid ridges.
In one embodiment, the top ridges are coated with n-type dopant liquid/paste (such as phosphorus); the rear ridges are coated with p-type dopant liquid/paste (such as boron). The 3-D TFSC substrate 642 is shown moving in 644 on input conveyor belt 646. Liquid film dispenser containing n-type liquid dopant source 682 applies a controlled thickness n-type liquid dopant film 684. This n-type dopant liquid comes from n-type liquid dopant source and liquid level and depth controller 686. Liquid film dispenser containing p-Type liquid dopant source (with peripheral air levitation) 688 applies a controlled thickness p-type liquid dopant film 690. This p-type dopant liquid comes from p-type liquid dopant source and liquid level and depth controller 692. The 3-D TFSC substrate 642 next moves into the curing area where the dopant liquid/paste layers are concurrently formed using a curing lamp 656 which uses IR or UV curing beams 658. The 3-D TFSC substrate 642 is next shown moving out 660 to the output conveyor belt 662, which may move the substrate 642 to an in-line diffusion furnace, where the n+ and p+ contacts and selective emitter regions are concurrently formed.
As in the setups in
The following section shows cross-sectional views of the TFSC substrate during various stages of the process flows outlined above. In the following FIGURES, the relative dimensions are not shown to scale.
The following FIGURES show alternative views, corresponding to various steps in the process flows for fabrication of TFSCs outlined above.
The previous section illustrated a preferred embodiment of a hexagonal-pyramid TFSC substrate. Alternative embodiments may use alternative designs for the unit cells such as inverted pyramid unit cells with polygon bases, including square pyramid, triangular pyramid, etc.; other embodiments may include 3-D TFSC substrates with V-groove or orthogonal V-groove patterns, etc. For example,
In the following section, alternative embodiments of process flows for fabricating templates using either lithography and etch techniques or laser micromachining (or laser drilling) are described. The templates are then used and reused numerous times to fabricate the 3-D TFSC substrates for 3-D TFSC fabrication.
Templates may be fabricated using electronic-grade silicon wafers, solar-grade silicon wafers, or lower-cost metallurgical-grade silicon wafers. Moreover, templates made of silicon can be fabricated either using monocrystalline or multicrystalline silicon wafers. The starting template wafer may either be a standard polished wafer (after saw damage removal) or even a lower grade wafer immediately after wire sawing (without saw damage removal). The latter may further reduce the cost of the templates. The relatively low cost of each template is spread over numerous 3-D TFSC substrates, resulting in much lower TFSC substrate and finished module costs compared to the standard state-of-the-art (e.g., 200 microns thick) solar-grade monocrystalline and multicrystalline silicon wafers and associated modules.
For further explaining how a template is fabricated,
An alternative embodiment of a process flow 894 for patterning of a template is outlined in
The following section outlines various process flows for fabricating 3-D pyramidal TFSC substrates using the templates described above.
Depending on the emitter doping type (n-type or p-type), the in-situ base doping type is chosen to be p-type (e.g., boron) or n-type (e.g., phosphorus). The embodiments shown provide examples of boron-doped hexagonal-pyramid 3-D TFSC substrates which may be used to fabricate TFSCs with n-type, phosphorus-doped selective emitters. In an alternative embodiment, all the doping polarities may be inverted, resulting in phosphorus-doped hexagonal-pyramid 3-D TFSC substrates which may be used for fabricating cells with boron-doped selective emitters.
In the next section, various embodiments of this disclosure for making solar modules suitable for building rooftops and façades, centralized power generation, and other applications are described. Usually solar modules are made by arranging a plurality of solar cells and connecting them in series (series electrical connections) within a solar module assembly protected by a top glass layer and a rear protective material layer such as Tedlar. The cells may be connected in series in order to step up the DC voltage (while maintaining the solar module current at the same level at the level of the cell current) to facilitate high-efficiency DC-to-AC power conversion.
The solar module structures and assembly methods of this disclosure are based on the use of a printed-circuit board (PCB) to assemble the 3-D TFSCs in a closely packed array and to connect the cells (in one embodiment in series) using the PCB plate within a module assembly. The PCB plate may have a single patterned metal (in one embodiment, copper) interconnect layer on the top of the PCB or two patterned copper layers on the top and rear surfaces of the PCB plate.
The 3-D TFSC substrates of this disclosure may utilize peripheral thick silicon frames, both for added mechanical support and also to facilitate formation of wrap-through or wrap-around emitter contact metallization (for ease of solar module assembly). The thick silicon frame may be separately made from very low-cost silicon material (such as metallurgical grade or reclaim silicon wafers).
These slivers 1056 may be used to make the thick silicon frames for the substrates shown above. The separately fabricated thick silicon frame may then be integrally attached to the 3-D TFSC substrates, in embodiment before 3-D thin-film cell processing, by one of the following techniques: electron-beam welding at several peripheral spots/junctions; attachment during the 3-D TFSC substrate fabrication silicon deposition by placing the peripheral thick silicon frame on the template and allowing seamless attachment of the thick silicon frame to the 3-D TFSC substrate by the silicon deposition process; or a clean cured epoxy.
Top view 1058 shows a thick silicon frame to be fused to the 3-D TFSC substrate. The silicon frame thickness 1060 is roughly 50 to 500 microns. There are welded (e.g., e-beam-welded) joints 1062 (four welded joints), where L 1064 is roughly 150 to 300 millimeters, and where W 1066 is roughly 100 to 1000 microns. The slivers 1056 may also have through-holes (shown in view 1068) to help with the wrap-through/wrap-around emitter metallization contacts.
The following section outlines various calculations related to the disclosed subject matter.
For given thin silicon film thickness and substrate size (e.g., 200 mm×200 mm substrate size) values, the actual amount (e.g., amount as measured by the total silicon surface area, volume, or weight) of silicon material used in the 3-D hexagonal-pyramid substrate structure is actually larger than that of a co-planar (flat) substrate with the same dimensions (e.g., 200 mm×200 mm).
Frontside aperture angle α is the angle defined by A-T-B, and frontside aperture angle β is the angle defined by H6-T-H3, and can be calculated as follows:
β=2 tan−1 [d/(2H)]
The surface area of the cone pyramid base (Shb)
S hb=[(3√3)/8]·d 2
The surface area of the cone pyramid sidewall (Shp)
S hp=[(3√3)/8]·d 2·√[1+( 16/3)·(H/D)2]
Therefore, the effective surface area enlargement factor (Shp/Shb) is:
S hp /S hb=√[1+( 16/3)·(H/d)2]
To achieve very efficient light trapping within the 3-D TFSC structure and very low effective surface reflectance with a reasonable (i.e., not excessive) area enlargement factor of Shp/Shb, the aperture angles (α and β) are chosen to be preferably in the range of around 20° to around 40°.
φ=2 tan−1 [D/(2H)]
The surface area of cone pyramid base (Scb) is:
S cb=(πD 2)/4
The surface area of cone pyramid sidewall (Scp) is:
S cp=[(πD 2)/4]·√[1+(2H/D)2]
Therefore, the ratio of the sidewall surface area Scp to the top base surface area Scb is:
S cp /S cb=√[1+(2H/D)2]
One important consideration in the TFSC and module interconnects is the total power loss associated with the electrical interconnects in the TFSCs and the solar module assembly. The hexagonal-pyramid 3-D c-Si TFSC and PCB-based module designs of this disclosure effectively address this issue, resulting in very low interconnect ohmic losses in the cells and within the module. This feature (in conjunction with the highly efficient packing of the TFSCs on the PCB-based solar module assembly) substantially narrows the efficiency gap between the TFSCs and the solar module assembly in the technology of this disclosure.
The next section relates to the basic calculations of the emitter contact metallization ohmic losses in the hexagonal-pyramid 3-D TFSCs of this disclosure. The calculations of ohmic losses for emitter contact metallization are also applicable to the base contact metallization. However, since several embodiments of this disclosure mount the 3-D TFSCs on patterned printed circuit boards (PCBs), the base contact metallization is electrically connected in a planar format to a very high conductivity copper pad; this substantially reduces the base interconnect ohmic losses (compared to the emitter interconnect ohmic losses). Therefore, in practical embodiments of this disclosure, the interconnect ohmic losses are dominated by the emitter contact metallization.
For the following calculations: I0 is the total cell current at peak power; A=(πA2)/4, total cell area (shown for round cell); J0=(4·I0)/(πa2), cell current density; Rthm is the sheet resistance of top honeycomb contact metal; C is the effective flat surface coverage of honeycomb contact with vertical height L; and Reff=Rthm/C, where Reff is the effective flat surface sheet resistance of top metal contact.
Based on this, the interconnect ohmic losses as maximum cell power are:
The following FIGURES show plots for various values of Rthm and L/H.
In summary, the disclosed subject matter provides multiple embodiments of pyramidal three-dimensional thin-film solar cells. The pyramidal three-dimensional thin-film solar cell comprises a semiconductor substrate with self-aligned selective emitter regions and self-aligned base diffusion regions. The pyramidal three-dimensional thin-film solar cell further includes self-aligned emitter contact metallization regions and self-aligned base contact metallization regions.
The foregoing description of the preferred embodiments is provided to enable any person skilled in the art to make or use the claimed subject matter. Various modifications to these embodiments will be readily apparent to those skilled in the art, and the generic principles defined herein may be applied to other embodiments without the use of the innovative faculty. Thus, the claimed subject matter is not intended to be limited to the embodiments shown herein but is to be accorded the widest scope consistent with the principles and novel features disclosed herein.
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|Classification aux États-Unis||136/255, 136/256, 136/261|
|Classification coopérative||H01L31/056, H01L31/00, H01L31/048, Y02E10/52, H01L31/0504, H01L31/022425, H01L31/1896, H01L31/0547, H01L31/035281, H01L31/046, Y02B10/12|
|Classification européenne||H01L31/18, H01L27/142R2, H01L31/042|
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